Method and apparatus for generating thz radiation
a radiation generation and thz technology, applied in non-linear optics, instruments, optics, etc., can solve the problems of not being able to devise a design capable of such drastic cascading or changing the position of the spectrum, and the generation of such large number of lines. to achieve the effect of increasing the conversion efficiency and/or output power of thz radiation
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first embodiment
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[0086]Features of the first embodiment of the invention are described with reference to FIGS. 1 to 13.
[0087]FIG. 1 shows a schematic of the THz source apparatus 100 comprising an input radiation source device 10 for generating optical input radiation, an imaging system 20 and a first conversion crystal device 30 for THz generation. The input radiation source device 10 comprises of a pump system with an optical pump source 11 creating a first radiation component and an optical seed source 12 creating a second radiation component. In this case, the THz source apparatus 100 is called Type O THz-COPA. In an alternative case (see FIG. 7), a THz seed source 13 is employed, and the THz source apparatus 100 is called Type T THz-COPA. Various possible implementations for the optical pump source 11 and optical seed source 12 are described below.
[0088]The imaging system 20 (details not shown) comprises refractive and / or reflective optics as well as a beam combiner unit, e.g., b...
second embodiment
of the Invention
[0114]Features of the second embodiment of the invention are described with reference to FIGS. 14 to 17.
[0115]FIG. 14 shows a schematic illustration of the THz source apparatus 100 comprising an input radiation source device 10 for generating multi-pulse optical input radiation, an imaging system 20 and a first conversion crystal device 30 for THz generation. The input radiation source device 10 is adapted for creating a sequence of ultrashort pulses having a temporal separation (Δt) equal to an integer multiple of a reciprocal of the THz frequency of the THz radiation to be generated (Δt=N·1 / fTHz, N=1, 2, . . . ). With this embodiment, the multi-line frequency spectrum is provided by the optical input radiation in the first conversion crystal device 30.
[0116]The temporal pulse format and corresponding spectrum of the optical input radiation in frequency domain is illustrated in FIG. 15. The temporal pulse format (FIG. 15B) is a sequence of ultrashort pulses in which...
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